This paper is archived as a speculative research work. This paper derives the Pauli exclusion principle for completed EAS electron supports from finite scalar-field structure. The derivation begins with the completed electron support Sₑ^ (j) = GₑA union GₑB union j₀, j₁, j₂, whose three completed channels determine a report space R³ = R (1, 1, 1) (+) Z. The common-mode line supplies the charge-facing channel, while the zero-sum plane Z = (P₀, P₁, P₂): P₀ + P₁ + P₂ = 0 supplies the finite SOO sign sector. Using the phase-specific difference report partialFᵖhi and the quadratic SOO report operator KFᵖhi = (partialFᵖhi) * partialFᵖhi, the zero-sum sector supports the double-cover sign pattern on channel-visible eigenspaces satisfying the SOO half-period condition, z₄₋₋ + ₓ = -z₄₋₋, z₄₋₋ + ₂ₓ = z₄₋₋. This finite sign sector yields an EAS spin-statistics bridge: complete electron two-support states lie in the exterior support-frame sector wedge² Hₑᵖhi. Consequently, if two attempted electron supports have the same complete state h in Hₑᵖhi, their two-support frame is degenerate: h wedge h = 0. Thus the scalar fields admit no nondegenerate two-electron state in which two identical electron supports occupy the same complete state. This is the Pauli exclusion principle in scalar-field form. The result is not an interface-readout failure; it is a finite scalar-field admissibility result: duplicate complete electron states determine a degenerate two-support frame, equivalently a zero exterior report.
Michael Labhard (Mon,) studied this question.